2010
DOI: 10.1002/aic.12223
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An exact method for determining local solid fractions in discrete element method simulations

Abstract: A novel solid fraction algorithm is presented which accounts for the partial volume of a sphere straddling cuboidal bin boundaries. The algorithm accounts for spheres intersecting a single plane (face), two perpendicular planes (edge), or three perpendicular planes (corner). Comparisons are made against the more common algorithm in which the solid fraction is determined by assigning the sphere's total volume to the bin in which the sphere's center of volume (COV) is located. Bin size-to-sphere diameter ratios … Show more

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Cited by 28 publications
(18 citation statements)
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“…This calculation is handled by a void fraction scheme. The void fraction within a fluid cell may be determined exactly 3 . However, such a calculation may require a complicated mathematical model and considerable computational expense, especially for complex geometries, nonspherical particles, and unstructured CFD grids.…”
Section: Introductionmentioning
confidence: 99%
“…This calculation is handled by a void fraction scheme. The void fraction within a fluid cell may be determined exactly 3 . However, such a calculation may require a complicated mathematical model and considerable computational expense, especially for complex geometries, nonspherical particles, and unstructured CFD grids.…”
Section: Introductionmentioning
confidence: 99%
“…A lower value for Δx is not desirable in CFD-DEM simulations because as the CFD cell size approaches the particle diameter, accurate calculation of local porosity is compromised due to reduced statistical averaging among particles inside the CFD cell [27], which may result in incorrect values in computation of gas-solid drag terms and numerical instabilities in solving the fluid-phase equations [4]. Eq.…”
Section: Total Number Of Particles N Pmentioning
confidence: 99%
“…If a part of a nanosphere's volume is located outside the box, we calculate the corresponding partial volume (δVout,i) using the analytical expressions from. [ 38 ] Every time the sum of the partial volumes that are located outside of the box (ΔVout=iδVout,i) exceeds the volume of one nanosphere, we then place one additional nanosphere into the box. The total number of particles hence is Ntot=N0+normalΔVoutVscat, where corresponds to the floor operator.…”
Section: Numerical Modeling Of Optical Materialsmentioning
confidence: 99%